US8575662B2

US8575662B2 - Solid state imaging device having high pixel density

Info

Publication number: US8575662B2
Application number: US13/043,081
Authority: US
Inventors: Fujio Masuoka; Nozomu Harada
Original assignee: Unisantis Electronics Singapore Pte Ltd
Current assignee: Unisantis Electronics Singapore Pte Ltd
Priority date: 2010-03-08
Filing date: 2011-03-08
Publication date: 2013-11-05
Anticipated expiration: 2031-03-08
Also published as: WO2011111662A1; CN102334189B; KR20110124267A; CN102334189A; JPWO2011111662A1; KR101211442B1; JP4912513B2; TW201143070A; US20110215381A1

Abstract

Each pixel of a solid state imaging device comprises a first semiconductor layer formed on a substrate, having a first-conductive type; a second semiconductor layer formed thereon, having a second-conductivity type; a third semiconductor layer formed in the upper side of the second semiconductor layer, having the first-conductivity type; a fourth semiconductor layer formed in the outer side of the third semiconductor layer, having the second-conductivity type; a gate conductor layer formed on the lower side of the second semiconductor layer via an insulating film; and a fifth semiconductor layer formed on the top surfaces of the second semiconductor layer and third semiconductor layer, having the second-conductivity type, wherein the fifth semiconductor layer and fourth semiconductor layer are connected to each other, and at least the third semiconductor layer, upper region of the second semiconductor layer, fourth semiconductor layer, and fifth semiconductor layer are formed in an island.

Description

RELATED APPLICATIONS

Pursuant to 35 U.S.C. §119(e), this application claims the benefit of the filing date of Provisional U.S. Patent Application Ser. No. 61/311,507 filed on Mar. 8, 2010. This application also claims priority under 35 U.S.C. §119(a) to JP2010-050675 filed on Mar. 8, 2010 and JP2010-253589 filed on Nov. 12, 2010. The entire contents of these applications are hereby incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a solid state imaging device and particularly to a solid state imaging device having reduced residual images, dark current, noise, mixed color, and a high pixel density.

2. Description of the Related Art

Currently, CCD and CMOS solid state imaging devices are extensively used in various video cameras and still cameras. Improvement in performance of solid state imaging devices, such as higher resolutions and higher sensitivity, is always demanded. Technical innovations for higher pixel densities have been made to realize higher resolution solid state imaging devices. Furthermore, technical innovations for lower noise have been made to realize highly sensitive solid state imaging devices.

A prior art solid state imaging device is disclosed in K. Yonemoto, H. Sumi, R. Suzuki, T. Ueno's: “A CMOS Image Sensor with a Simple FPN-Reduction Technology and a Hole Accumulated Diode,” 2000 IEEE International Solid-State Circuits Conference, Digest Papers, MP6. 1 (2000). This prior art CMOS solid state imaging device is shown in FIG. 24A. FIG. 24A is an illustration showing the structure of a pixel of the CMOS solid state imaging device. The CMOS solid state imaging device comprises a PN photodiode PD, a transfer gate TG joined to the PN photodiode PD, a floating diode FD joined to a channel 20 below an electrode of the transfer gate TG, an amplifying MOS transistor 21, a first pixel selection MOS transistor 22 connected to the amplifying MOS transistor 21, a reset MOS transistor 23, and a second pixel selection MOS transistor 24 connected to the transfer gate TG. The PN photodiode PD has a photodiode surface P⁺ layer 19 on the surface of a photodiode N layer 27. The photodiode surface P⁺ layer 19 is connected to a channel stopper P⁺ layer 18. The amplifying MOS transistor 21 has a gate AG connected to the floating diode FD. The reset MOS transistor 23 has a reset gate RG (n) connected to the floating diode FD and a reset drain RD diode. The gates of the first and second pixel

selection MOS transistors

22 and 24 are connected to a column scanning circuit joined to a column selection line RL (m). A row selection line CL (n) joined to the source of the second pixel selection MOS transistor 24 and the gate RG (n) of the reset MOS transistor 23 are connected to a row scanning circuit. The reset drain RD of the reset MOS transistor 23 and the drain of the amplifying MOS transistor 21 are connected to a power supply line at voltage V_dd. The source of the first pixel selection. MOS transistor 22 is connected to a signal line 25.

Signal charges (electrons in this case) generated by light irradiation are accumulated in the PN photodiode PD. The accumulated signal charges are transferred to the floating diode FD when an ON voltage is applied to the transfer gate TG. The potential of the floating diode FD changes according to the signal charge packets. At the same time, the gate voltage of the amplifying MOS transistor 21 connected to the floating diode FD changes according to the signal charge packets. When an ON voltage is applied to the gate of the first pixel selection MOS transistor 22, a signal current according to the gate voltage of the amplifying MOS transistor 21 that has changed according to the signal charge packets runs through the signal line 25. The current is read as an output.

FIG. 24B shows the potential profile along a section line A-A in FIG. 24A when an ON voltage is applied to the transfer gate TG and the signal charges accumulated in the photodiode PD are transferred to the floating diode FD. In FIG. 24B,

signal charges

26 a, 26 b, and 26 c are shown by hatching for distinction. The signal charges 26 a accumulated in the photodiode PD are transferred to the floating diode FD. The signal charges 26 b transferred from the floating diode FD modulate the gate voltage of the amplifying MOS transistor 21. Here, among the deepest potential Φ_mpin the photodiode PD when there is no signal charge, the potential Φ_tgof the channel 20 when an ON voltage is applied to the transfer gate TG, and the potential Φ_fgof the floating diode FD when there is no transferred signal charge, Φ_fgis the deepest, Φ_tgis the second deepest, and Φ_mgis the shallowest. The signal charges consist of electrons in the pixel, establishing the relationship Φ_fg>Φ_tg>Φ_mp. The channel stopper P⁺ layer 18 has a potential of 0 V. The potential profile relationship allows most signal charges in the photodiode PD to be transferred to the floating diode FD. Consequently, trailing residual images can be prevented when images of moving objects are captured. Furthermore, the above structure can prevent kTC noise, which otherwise causes deteriorated sensitivity. The signal charges 26 b in the floating diode FD are removed through the reset drain RD when a voltage is applied to the reset gate RG (n). In such a case, a certain level of charges 26 c remains in the floating diode FD.

The signal charges can completely be transferred from the photodiode PD to the floating diode FD when the P⁺ layer 19 on the surface of the N layer 27 of the photodiode PD (“the photodiode surface P⁺ layer” hereafter) is connected to the channel stopper P⁺ layer 18 to which 0 V is applied so that the photodiode surface P⁺ layer 19 is fixed (pinned) to 0 V. FIG. 24C shows the potential profile through the SiO₂film, photodiode surface P⁺ layer 19, photodiode N layer 27, and photodiode P layer 28 along a section line B-B in FIG. 24A. FIG. 24C shows signal charges 26 d by hatching for distinction. The deepest potential Φ_mpin the photodiode PD when there is no signal charge is within the photodiode N layer 27. Therefore, the signal charges 26 d are present in the inner photodiode N layer 27 and photodiode P layer 28 rather than in the photodiode surface P⁺ layer 19 of which the potential is pinned. Holes 29 are accumulated in the photodiode surface P⁺ layer 19. The holes 29 are recombined to electrons thermally excited due to the SiO2-Si interface states and prevent the electrons infusing into the signal charges 26 d, and no dark current occurs.

If the CMOS solid state imaging device shown in FIG. 24A does not have the photodiode PD surface P⁺ layer 19 joined to the channel stopper P⁺ layer 18 having a fixed potential of 0V, the photodiode PD can directly be connected to the gate AG of the amplifying MOS transistor 21. In this way, the voltage of the gate AG of the amplifying MOS transistor 21 can directly be changed according to the signal charges accumulated in the photodiode PD for imaging operation. However, such a structure may cause residual images and increase kTC noise and dark current as mentioned above. On the other hand, the photodiode PD surface P⁺ layer 19 does not allow a contact hole to be formed on the photodiode PD so as to connect the photodiode PD to the gate AG of the amplifying MOS transistor 21 via metal wiring through the contact hole. Therefore, the transfer gate TG and floating diode FD have to newly be added. Such newly added regions hamper increase in the pixel density.

Other problems of prior art CMOS solid state imaging devices include deteriorated resolution and mixed color in color imaging.

SUMMARY OF THE INVENTION

The present invention is made in view of the above circumstances and has the objective of realizing a solid state imaging device having reduced residual images, dark current, and noise, and a high pixel density. Another purpose of the present invention is to realize a solid state imaging device preventing deteriorated resolution and mixed color in color imaging.

In order to achieve the above purposes, the solid state imaging device of the present invention is a solid state imaging device including one or multiple pixels, each of the pixels comprising a first semiconductor layer formed on a substrate, a second semiconductor layer formed on the first semiconductor layer, a first insulating film formed on a lower side of the second semiconductor layer, a gate conductor layer formed on the lower side of the second semiconductor layer via the first insulating film, a third semiconductor layer formed in an upper side of the second semiconductor layer, a fourth semiconductor layer formed on a side of the third semiconductor layer that is not facing a side of the second semiconductor layer, and a fifth semiconductor layer formed on top of the second semiconductor layer and the third semiconductor layer, the fifth semiconductor layer electrically connected to the fourth semiconductor layer, wherein at least the third semiconductor layer, the upper region of the second semiconductor layer where the third semiconductor layer is formed, the fourth semiconductor layer, and the fifth semiconductor layer are formed in an island, a diode comprises the second semiconductor layer and the third semiconductor layer, a junction transistor comprises the diode serving as a gate thereof and the second semiconductor layer serving as a channel thereof, the channel being between the first semiconductor layer and the fifth semiconductor layer, a MOS transistor comprises the second semiconductor layer serving as a channel thereof between the first semiconductor layer and the third semiconductor layer and the gate semiconductor layer functioning as a gate thereof, a signal charge generated by a electromagnetic energy wave is accumulated in the diode, current flowing to the junction transistor and changing in accordance with amount of the signal charge accumulated in the diode is detected as a signal, the signal charge accumulated in the diode is removed at the first semiconductor layer through the MOS transistor channel, the fourth semiconductor layer and the fifth semiconductor layer have same voltage.

Preferably, the solid state imaging device of the present invention further comprises a first conductor layer formed on the side of the fourth semiconductor layer via the first insulating film so as to enclose the third semiconductor layer, the upper region of the second semiconductor layer, and the fourth semiconductor layer in the shape of an island, the first conductor layer including a light-blocking conductive material, wherein the first conductor layer is connected to the fifth semiconductor layer.

The present invention provides a solid state imaging device having reduced residual images, dark current, and noise and a high pixel density.

A light-blocking layer is provided to enclose the semiconductor layer in the shape of an island, whereby mixed color and deteriorated resolution can be prevented.

BRIEF DESCRIPTION OF THE DRAWINGS

A more complete understanding of this application can be obtained when the following detailed description is considered in conjunction with the following drawings, in which:

FIG. 1A is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 1 of the present invention;

FIG. 1B is an illustration showing the pixel structure of a solid state imaging device according to a modified example of Embodiment 1 of the present invention.

FIG. 2 is an illustration showing the circuit configuration of a solid state imaging device according to Embodiment 1;

FIG. 3A is an illustration showing a pixel structure for explaining Embodiment 1;

FIG. 3B is an illustration showing a potential profile for explaining Embodiment 1;

FIG. 3C is an illustration showing a pixel structure for explaining Embodiment 1;

FIG. 3D is an illustration showing a potential profile for explaining Embodiment 1;

FIG. 3E is an illustration showing a potential profile for explaining Embodiment 1;

FIG. 4A is an illustration showing a pixel structure for explaining Embodiment 1;

FIG. 4B is an illustration showing a potential profile for explaining Embodiment 1;

FIG. 4C is an illustration showing a potential profile for explaining Embodiment 1;

FIG. 5A is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 2 of the present invention;

FIG. 5B is an illustration showing a pixel structure for explaining Embodiment 2;

FIG. 5C is an illustration showing a pixel structure for explaining Embodiment 2;

FIG. 6 is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 3 of the present invention;

FIG. 7 is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 4 of the present invention;

FIG. 8 is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 5 of the present invention;

FIG. 9 is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 6 of the present invention;

FIG. 10 is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 7 of the present invention;

FIG. 11 is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 8 of the present invention;

FIG. 12 is an illustration showing the pixel structure of a solid state imaging device according to Embodiment 9 of the present invention;

FIG. 13 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 14 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 15 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 16 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 17 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 18 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 19 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 20 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 21 is an illustration for explaining a method of producing the solid state imaging device according to Embodiment 9;

FIG. 22 is a cross-sectional view of a solid state imaging device according to Embodiment 10 of the present invention;

FIG. 23 is a cross-sectional view of a solid state imaging device according to Embodiment 11 of the present invention;

FIG. 24A is an illustration showing a pixel structure for explaining a prior art solid state imaging device and its operation;

FIG. 24B is an illustration showing a potential profile for explaining a prior art solid state imaging device and its operation;

FIG. 24C is an illustration showing a potential profile for explaining a prior art solid state imaging device and its operation; and

FIG. 25 is an illustration showing a pixel structure for explaining a second prior art solid state imaging device

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Embodiments of the present invention will be described hereafter with reference to FIGS. 1A to 23.

Embodiment 1

A solid state imaging device 100 according to Embodiment 1 of the present invention will be described hereafter with reference to FIGS. 1A to 4.

The solid state imaging device 100 according to this embodiment has the basic pixel structure similar to that of the solid state imaging device described in International Publication No. WO 2009/034623, the content of which is entirely incorporated herein by reference.

FIG. 1A shows the pixel structure of the solid state imaging device 100 according to Embodiment 1. An individual pixel 11 has a first semiconductor N⁺ layer 1 formed on a substrate and the first semiconductor N⁺ layer 1 is connected to a wire XL extending in a first scanning direction. A MOS transistor 111 comprising a second semiconductor P layer 2 having an opposite conductivity type, insulating

film

3 a, 3 b, and

gate conductor layer

4 a, 4 b is formed on the first semiconductor N⁺ layer 1. A photodiode 112 consisting of the second semiconductor P layer 2 and a

third semiconductor layer

5 a, 5 b is formed to join to the MOS transistor 111. A fourth semiconductor P⁺ layer 6 a, 6 b is formed on the surface of the photodiode 112. A fifth semiconductor P⁺ layer 7 is formed to join to the fourth semiconductor P⁺ layer 6 a, 6 b. The fifth semiconductor P⁺ layer 7 is connected to a wire YL extending in the direction orthogonal to the first scanning direction. At least the region where the photodiode 112 is formed (the upper region of the second semiconductor P layer 2 where the third

semiconductor N layer

5 a, 5 b is formed and the third

semiconductor N layer

5 a, 5 b), fourth semiconductor P⁺ layer 6 a, 6 b, and fifth semiconductor P⁺ layer 7 are formed in the shape of an island. In this embodiment, the wire XL is a signal line and the wire YL is a pixel selection line. However, the combination of the wires XL and YL can be allowed to be a pixel selection line and a signal line, respectively.

In Embodiment 1, the second semiconductor layer is a P layer 2 made of a P type conductivity semiconductor. However, as illustrated in FIG. 1B, an i layer 2 i made of an intrinsic type semiconductor layer can be used instead of the P layer 2. An intrinsic semiconductor is a semiconductor made of substantially a single element. Although an intrinsic semiconductor is made without including impurities, it is inevitable that a tiny amount of impurity exists. As long as the intrinsic semiconductor layer containing an i layer 2 i does not impede the function of the solid state imaging device 100, it can contain a small amount of acceptor or donor impurity. With this type of configuration, a photodiode can be formed by the third semiconductor N layers 5 a, 5 b and the second semiconductor i layer 2 i. When sufficient voltage is applied between the fifth semiconductor P⁺ layer 7 and the signal line N⁺ layer 1, the fifth semiconductor P⁺ layer 7 hole flows towards the signal line N⁺ layer 1 according to the potential gradient generated within the second semiconductor i layer 2 i. In this way, the second semiconductor i layer 2 i functions as a junction transistor channel similarly to the second semiconductor P layer 2 in FIG. 1A.

FIG. 2 shows an exemplary circuit configuration of the solid state imaging device 100 according to this embodiment. The solid state imaging device 100 primarily comprises multiple pixels 11 a to 11 d arranged in a two-dimensional matrix, a vertical scanning circuit 201, a horizontal scanning circuit 202, a reset circuit 203, pixel selection lines YL1 and YL2, signal lines XL1 and XL2, reset lines RSL, signal line MOS transistors Tr1 and Tr2, and a correlated double sampling (CDS) output circuit 204. This embodiment will be described as a case in which the pixels are arranged in two rows and two columns. However, the solid state imaging device of the present invention is not restricted to this case.

As shown in FIG. 2, the vertical scanning circuit 201 supplying pixel selection signals to the pixels 11 a to 11 d are connected to the pixels 11 a to 11 d via the pixel selection lines YL1 and YL2 on a row basis. The pixels 11 a to 11 d are also connected to the CDS output circuit 204 via the signal lines XL1 and XL2 on a column basis. The gate electrodes of the signal line MOS transistors Tr1 and Tr2 arranged on the individual signal lines are connected to the horizontal scanning circuit 202 supplying signals for selecting signal lines to these gate electrodes. The signal lines XL1 and XL2 are also connected to switching parts SW1 and SW2, respectively. The gate conductor layers 4 a, 4 b of the MOS transistors 111 for reset operation are connected to the reset circuit 203 supplying reset signals to the gate conductor layers 4 a, 4 b via the reset lines RSL. With operation of the above circuit configuration, the signal currents of the pixels 11 a to 11 d are read from the CDS output circuit 204 in sequence.

Basic operation of the solid state imaging device 100 according to this embodiment will be described hereafter with reference to FIGS. 2 to 4. In the potential profiles of FIGS. 3 and 4, the accumulated signal charges are shown by hatching for distinction.

The basis operation of the solid state imaging device 100 comprises signal charge accumulation, signal reading, and reset. In the signal charge accumulation operation, signal charges generated by light irradiation are accumulated in the third

semiconductor N layer

5 a, 5 b and the second semiconductor P layer 2 near the third

semiconductor N layer

5 a, 5 b (“the photodiode region” hereafter). In the signal reading operation, a current running between the second semiconductor P layer 2 near the first semiconductor N⁺ layer 1 and the fifth semiconductor P⁺ layer 7 is measured so that the accumulated signal charge (packets) are measured. The current running between the second semiconductor P layer 2 near the first semiconductor N⁺ layer 1 and the fifth semiconductor P⁺ layer 7 varies according to the signal charge (packets) accumulated in the photodiode region. Therefore, the accumulated signal charge packets can be measured by measuring this current. In the reset operation, an ON voltage is applied to the

gate conductor layer

4 a, 4 b of the MOS transistor 111 to create a channel between the first semiconductor N⁺ layer 1 and the third

semiconductor N layer

5 a, 5 b. Consequently, the signal charges accumulated in the photodiode region are discharged to the first semiconductor N⁺ layer 1 and removed from the photodiode.

FIG. 3A is a schematic illustration showing the pixel structure when no signal charge is accumulated in the photodiode region during the signal reading. Here, the photodiode 112 has depleted

layer

8 a, 8 b as marked by broken lines. In this embodiment, when no signal charge is accumulated in the photodiode region, the depleted

layer

8 a, 8 b of the photodiode 112 is formed in a part of the upper region of the second semiconductor P layer 2 where the photodiode 112 is formed.

FIG. 3B shows the potential profile along the line A-A in FIG. 3A. During the signal reading, the potentials are set so that they become deeper in the following order: the potential of the first semiconductor N⁺ layer 1 (V_XLR), the potential of the fifth semiconductor P⁺ layer 7 (V_YLR), and the deepest potential Φ_PRin the third

semiconductor N layer

5 a, 5 b when no signal charge is accumulated. Signal charges in this embodiment consist of electrons. Therefore, the potentials are set to satisfies the relationship Φ_PR>V_YLR>V_XLR.

The photodiode surface P⁺ layer (the fourth semiconductor P⁺ layer) 6 a, 6 b are electrically connected to the fifth semiconductor P⁺ layer 7; therefore, the photodiode surface P⁺ layer 6 a, 6 b is at a potential V_YLR. Holes 29 are supplied from the fifth semiconductor P⁺ layer 7 and accumulated in the photodiode surface P⁺ layer 6 a, 6 b.

FIG. 3C is an illustration showing the pixel structure when signal charges are accumulated in the photodiode region during the signal reading. FIG. 3D shows the potential profile along the line A-A in FIG. 3C. During the signal reading, as shown in FIG. 3D, signal charges are accumulated in the photodiode region and the photodiode potential Φ_GRis changed according to the accumulated signal charges. Then, as shown in FIG. 3C, the width of the depleted

layer

8 a, 8 b is decreased according to the photodiode potential Φ_GRcreated by the accumulated signal charges. Subsequently, the width of the second semiconductor P layer 2 serving as the channel of an amplifying junction transistor is changed. Accordingly, the current running between the second semiconductor P layer 2 near the first semiconductor N⁺ layer 1 and the fifth semiconductor P⁺ layer 7 is changed.

FIG. 3E is a schematic illustration showing the potential profile along the line A-A in FIG. 3C when signal charges are further accumulated and excessive signal charge (packets) Q_exare accumulated in the photodiode region as accumulated signal charges in addition to the reading maximum signal charge (packets) Q_SRMduring the signal reading. In this embodiment, signal charges are accumulated in the photodiode region until the photodiode potential Φ_GRbecomes V_YLR. The excessive signal charge (packets) Q_exdue to extra light irradiation are recoupled to the holes 29 accumulated in the photodiode surface P⁺ layer 6 a, 6 b and disappear. In this embodiment, the potential relationship V_XLR<V_YLRis set; therefore, the excessive signal charge (packets) Q_exdo not migrate to the second semiconductor P layer 2. Consequently, excessive signal charges generated in the photodiode region by light irradiation can be removed without forming a drain particularly for removing excessive signal charges. Therefore, no excessive signal charges intrude into the channel of the amplifying junction transistor.

FIG. 4A is a schematic illustration showing the pixel structure including the depleted

layers

8 a and 8 b when no signal charge is accumulated in the photodiode region during the signal charge accumulation. In this embodiment, when no signal charge is accumulated in the photodiode region, the depleted

layer

8 a, 8 b of the photodiode 112 are formed in a part of the upper region of the second semiconductor P layer 2.

FIG. 4B shows the potential profile at the line A-A in FIG. 4A. For example, the potential V_XLRof the first semiconductor N⁺ layer 1 is set to 0 V, the potential V_YLRof the fifth semiconductor P⁺ layer 7 is set to 0 V, and the potential of the

gate conductor layer

4 a, 4 b of the MOS transistor 111 is set to 0 V during the signal charge accumulation. In this way, the accumulated signal charge (packets) Q_SSare accumulated in the photodiode region according to light irradiation as shown in FIG. 4B. If the accumulated signal charge packets Q_SSare larger than the reading maximum signal charge packets Q_SRM, excessive charges are recombined to the holes 29 accumulated in the fourth semiconductor P⁺ layer 6 a, 6 b and removed as described above upon transition to the signal reading operation.

FIG. 4C shows the potential profile at the line A-A in FIG. 1 during the reset. In the reset operation, the potentials are set so that they become deeper in the following order: the potential of the fifth semiconductor P⁺ layer 7 (V_YLR), the deepest potential Φ_PMin the third semiconductor N layers 5 a and 5 b when no signal charge is accumulated, the potential Φ_RGof the channel of the MOS transistor of the second semiconductor P layer 2 when an ON voltage is applied to the gate conductor layers 4 a and 4 b of the MOS transistor 111, and the potential of the first semiconductor N⁺ layer 1 (V_XLR). In this embodiment, the signal charges consist of electrons; the potentials are set to satisfy the relationship V_YLR<Φ_PM<Φ_RG<V_XLR. For example, V_YLR=0 V, V_XLR=2 V, and the voltage of the gate conductor layers 4 a and 4 b is 1.5 V. In this way, during the reset, the signal charges accumulated in the photodiode region do not stay in the photodiode region. Migrating to the first semiconductor N⁺ layer 1, the all signal charges are removed.

Consequently, residual images and kTC noise are prevented in the solid state imaging device shown in FIG. 24A.

Embodiment 2

FIGS. 5A to 5C are schematic illustrations of a pixel structure for explaining a solid state imaging device according to Embodiment 2 of the present invention. The same components as those of the solid state imaging device according to Embodiment 1 are referred to by the same reference numbers.

This embodiment is different from Embodiment 1 in that the depleted layer 8 c of the diode occupies the upper region of the second semiconductor P layer 2 where the photodiode 112 is formed when no signal charge is accumulated in the photodiode region as shown in FIG. 5A. Such a photodiode 112 is formed by properly adjusting the thicknesses and impurity concentrations of the third

semiconductor N layer

5 a, 5 b and second semiconductor P layer 2.

No channel is formed for running a current between the fifth semiconductor P⁺ layer 7 and the second semiconductor P layer 2 near the first semiconductor N⁺ layer 1 of the amplifying junction transistor when the depleted layer 8 c occupies the upper region of the second semiconductor P layer 2.

When signal charges are accumulated in the photodiode region, during the signal reading, the width (thickness) of the depleted

layer

8 a, 8 b of the photodiode 112 is decreased as shown in FIG. 5B. Therefore, the channel of the amplifying junction transistor is formed in the second semiconductor P layer 2, and a current according to the accumulated charges runs through the channel.

FIG. 5C is a schematic illustration showing the pixel structure including the depleted layer 8 c when no signal charge is accumulated in the photodiode region during the signal charge accumulation. During the signal charge accumulation, for example, the voltage V_XLRof the first semiconductor N⁺ layer 1 is set to 0 V and the voltage V_YLRof the fifth semiconductor P⁺ layer 7 is set to 0 V in a general practice.

As shown in FIG. 5C, the depleted layer 8 c of the photodiode 112 occupies the upper region of the second semiconductor P layer 2 when no signal charge is accumulated during the signal charge accumulation. The second semiconductor P layer 2 that is not occupied by the depleted layer 8 c allows signal charges generated in the second semiconductor P layer 2 to diffuse to and reach the fifth semiconductor P⁺ layer 7 or first semiconductor N⁺ layer 1. Consequently, the signal charges generated in the second semiconductor P layer 2 do not contribute to signals. On the other hand, the depleted layer 8 c occupying the upper region of the second semiconductor P layer 2 contributes to effective capture and accumulation of generated signal charges in the photodiode 112 particularly when a small quantity of light is irradiated.

Furthermore, when no signal charge is accumulated, the amplifying junction transistor channel is pinched off. Therefore, for example, the depleted layer 8 c serves to prevent injection of the holes 29 from the fifth semiconductor P⁺ layer 7 to the second semiconductor P layer 2 as a result of noise leaping to the pixel selection line YL other than during the signal reading.

As described above, during the signal reading, the depleted layer 8 c of the photodiode 112 occupies the upper region of the second semiconductor P layer 2 when no signal charge is accumulated in the photodiode region, providing a solid state imaging device having an excellent low irradiation property.

Embodiment 3

FIG. 6 is a cross-sectional view of two pixels for explaining a solid state imaging device according to Embodiment 3 of the present invention. The same components as those of the solid state imaging device according to Embodiment 1 are referred to by the same reference numbers. The components of a pixel 11 e are referred to by reference numbers with a suffix aa or ab and the components of a pixel 11 f are referred to by reference numbers with a suffix ba or bb. In the solid state imaging devices in

Embodiments

1 and 2, the

gate conductor layer

4 a, 4 b of the reset MOS transistor 111 is formed only on the channel of the MOS transistor 111. On the other hand, in the solid state imaging device according to this embodiment, gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb of the reset MOS transistors 111 are extended to cover photodiode surface P+ layers (the fourth semiconductor P⁺ layers) 6 aa, 6 ab, 6 ba, and 6 bb. Here, the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb enclose the pixel (island-shaped semiconductor) 11 e and 11 f, respectively. The gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb are made of, for example, a light-blocking conductive material such as polysilicon and metal, and absorb or reflect irradiated light.

Light (incident light) 10 a entering the first pixel 11 e from the front surface of the pixel (the top surface in FIG. 6) at an angle partly reaches the adjacent second pixel 11 f and generates signal charges in the above-described pixel structure according to Embodiment 1. This means that the signal charges originally to be generated in the first pixel 11 e leak into the adjacent pixel. Leakage of signal charges into an adjacent pixel may cause deteriorated resolution and mixed color particularly in a color imaging device in which each pixel is supposed to receive a predetermined color light. Deteriorated resolution and mixed color particularly in color imaging may lead to significant deterioration in image quality.

On the other hand, in this embodiment, the oblique incident light 10 a is absorbed or reflected by the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb made of a light-blocking material. The reflected light 10 c stays in the initial pixel 11 e and the above mentioned leakage of signal charges into the adjacent pixel 11 f does not occur.

In this embodiment, the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb are joined to the fifth semiconductor P⁺ layers 7 a and 7 b to which the voltage of the second wires YL3 and YL4 are applied. Therefore, the potential of the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb is fixed to the potential of the second wires YL3 and YL4. Because of the shield effect of the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb, the photodiode potential changing the channel width of the amplifying junction transistor is less affected by change with time of the potential of the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb of the reset MOS resistor, ensuring stable operation.

Embodiment 4

A solid state imaging device according to Embodiment 4 will be described hereafter with reference to FIG. 7. The same components as those of the solid state imaging device according to Embodiment 3 are referred to by the same reference numbers. In the above-described solid state imaging device according to Embodiment 3, the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb of the reset MOS transistors 111 are extended over the photodiode surface P⁺ layers (the fourth semiconductor P⁺ layers) 6 aa, 6 ab, 6 ba, and 6 bb. On the other hand, in the solid state imaging device according to this embodiment, first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb joined to the fifth semiconductor P⁺ layers 7 a and 7 b cover the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb. The first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb enclose the island-shaped

semiconductors

11 e and 11 f, respectively. The first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb are comprised of a light-blocking conductive material.

In this way, as in the solid state imaging device according to Embodiment 3, the incident light 10 a entering the first pixel 11 e from the front surface of the pixel at an angle is absorbed or reflected by the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb or the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb. The reflected light 10 c stays in the initial pixel 11 e and no leakage of signal charges into the adjacent pixel 11 f occurs.

Furthermore, in the above-described solid state imaging device according to Embodiment 3, the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb cover the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb. Although shielded by the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb fixed to the voltage of the wires YL3 and YL4, the photodiode potential changing the channel width of the amplifying junction transistor is easily affected by capacitive coupling following any change in voltage of the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb of the MOS transistors 111. On the other hand, in the solid state imaging device of this embodiment, the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb covering the photodiode surface are electrically connected to the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb, respectively, and equal in potential to the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb. Therefore, the potential of the photodiode surface P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb is less affected by change in voltage other than the wires YL3 and YL4. Consequently, the photodiode potential changing the channel width of the amplifying junction transistor stably operates and the solid state imaging device of this embodiment stably operates.

Embodiment 5

A solid state imaging device according to Embodiment 5 of the present invention will be described hereafter with reference to FIG. 8. The same components as those of Embodiment 4 are referred to by the same reference numbers. In a conventional two-dimensional solid state imaging device, the pixel selection line, pixel signal line, pixel power supply line, and gate of a pixel MOS transistor of each pixel are connected to a scanning circuit, power circuit, signal processing circuit, gate pulse generation circuit, and the like provided around the solid state imaging device. The connection lines are provided in a first wiring direction or in a second wiring direction. For example, the first semiconductor N⁺ layers 1 a and 1 b are connected to signal lines and the fifth semiconductor P⁺ layers 7 a and 7 b are connected to pixel selection lines. As shown in FIG. 8, when the signal lines XL3 and XL4 are provided in the vertical direction on the sheet, the pixel selection lines are generally provided in the horizontal direction on the sheet. In this case, the pixel selection lines consist of the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb connecting the fifth semiconductor P⁺ layers 7 a and 7 b and the first wiring conductor layers 14 a to 14 c connecting the first conductor layers 13 aa, 13 ba, 13 ba, and 13 bb of adjacent pixels. In this embodiment, the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb are connected to the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb of the adjacent pixels near the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb of the MOS transistors. Furthermore, the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb and first wiring conductor layers 14 a to 14 c are made of a light-blocking conductive material. In this embodiment, the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb and the first wiring conductor layers 14 a to 14 c are integrally formed.

With the above structure, as shown in FIG. 8, as in the solid state imaging devices according to Embodiments 3 and 4, the incident light 10 a entering the first pixel 11 e from the pixel front surface at an angle is absorbed or reflected by the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb or the gate conductor layers 4 aa, 4 ab, 4 ab, and 4 bb. The reflected light 10 c stays in the initial pixel 11 e and no leakage of signal charges into the adjacent pixel 11 f occurs. Furthermore, leakage of the light entering the space between the

pixels

11 e and 11 f into the second semiconductor P layers 2 a and 2 b through the gap between the first conductor layers 13 ab and 13 ba joined to the fifth semiconductor P⁺ layers 7 a and 7 b, respectively, and the gate conductor layers 4 ab and 4 ba of the MOS transistors is effectively prevented. As shown in FIG. 8, the light 16 once entering the pixel 11 e and emerging from the gap between the first conductor layer 13 ab and the gate conductor layer 4 ab is absorbed or reflected by the first wiring conductor layer 14 b. Therefore, leakage of such light into the second semiconductor P layer 2 b of the adjacent pixel 11 f through the gap between the first semiconductor layer 13 ba and gate conductor layer 4 ba of the adjacent pixel 11 f is effectively prevented. Unlike this embodiment, if the first conductor layer 13 ab is connected to the first conductor layer 13 ba connected to the fifth semiconductor P⁺ layer 7 b of the adjacent pixel at the top where a light enters, the light easily leaks into the adjacent pixel by coming around from between the pixel selection lines provided in the horizontal direction or through the gap between the gate conductor layers 4 ab and 4 ba and the first conductor layers 13 ab and 13 ba. In the solid state imaging device of this embodiment, the light leakage can effectively be prevented.

Embodiment 6

A solid state imaging device according to Embodiment 6 of the present invention will be described hereafter with reference to FIG. 9. The same components as those of Embodiment 4 are referred to by the same reference numbers. In the solid state imaging device of this embodiment, the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb of the MOS transistors 111 are provided in the horizontal direction in FIG. 9. Furthermore, the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb of the

pixels

11 e and 11 f are connected by the second wiring conductor layers 15 a to 15 c at the upper parts of the MOS transistors. The second wiring conductor layers 15 a to 15 c are made of a light-blocking conductive material. In this embodiment, the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb and the second wiring conductor layers 15 a to 15 c are integrally formed.

With the above structure, as shown in FIG. 9, the light 10 a entering the first pixel 11 e from the front surface of the pixel at an angle is absorbed or reflected by the first conductor layers 13 aa and 13 ba, or the gate conductor layers 4 aa and 4 ab, as in the solid state imaging devices of Embodiments 3 to 5. The reflected light 10 c stays in the initial pixel 11 e and no leakage of signal charges into the adjacent pixel 11 f occurs. As in the above-described solid state imaging device according to Embodiment 5, leakage of the light entering the space between the adjacent pixels into the second semiconductor P layers 2 a and 2 b of the adjacent pixels through the gap between the gate conductor layers 4 ab and 4 ba and the first conductor layers 13 ab and 13 ba is effectively prevented. Furthermore, the light 16 once entering the pixel 11 e and emerging from the gap between the gate conductor layer 4 ab and first conductor layer 13 ab is absorbed or reflected by the second wiring conductor layer 15 b. Therefore, leakage of such light into the second semiconductor P layer 2 b of the adjacent pixel through the gap between the gate semiconductor layer 4 ba and first conductor layer 13 ba of the adjacent pixel 11 f is effectively prevented.

Embodiment 7

A solid state imaging device according to Embodiment 7 of the present invention will be described hereafter with reference to FIG. 10. The same components as those of Embodiment 4 are referred to by the same reference numbers. This embodiment is different from Embodiment 4 in that the space between the

pixels

11 e and 11 f, namely both or one of the space between the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb and the space between the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb is filled with the filling conductor layers (the second conductor layer) 16 a to 16 c and 17 a to 17 c. In this embodiment, both the space between the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb and the space between the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb are filled with the filling conductor layers 16 a to 16 c and 17 a to 17 c. In such a case, the second wires YL3 and YL4 joined to the fifth semiconductor P⁺ layers 7 a and 7 b, respectively, and the gate conductor layers 4 aa, 4 ab, 4 ba, 4 bb of the MOS transistors 111 are provided in the same wiring direction. When the second wires YL3 and YL4 and the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb are provided in the wiring directions orthogonal to each other, either the space between the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb or the space between the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb will be filled with the conductor layers 16 a to 16 c or 17 a to 17 c in the figure.

The filling conductor layers 16 a to 16 c and 17 a to 17 c are made of a light-blocking conductive material. Therefore, for example, the light entering the space between the pixels is absorbed or reflected by the filling conductor layers 16 a to 16 c and 17 a to 17 c. Hence, leakage of light into an adjacent pixel can effectively be prevented as in the solid state imaging devices of Embodiments 5 and 6.

Embodiment 8

A solid state imaging device according to Embodiment 8 of the present invention will be described hereafter with reference to FIG. 11. The same components as those of Embodiment 4 are referred to by the same reference numbers. FIG. 11 is an enlarged view of a region including the second semiconductor P layer 2 a, gate conductor layer 4 ab, third semiconductor N layer 5 ab, fourth semiconductor P⁺ layer 6 ab, and fifth semiconductor P⁺ layer 7 a of the pixel structure of the solid state imaging device of Embodiment 4. This embodiment is different from Embodiment 4 in that the first conductor layer 13 ab joined to the fifth semiconductor P⁺ layer 7 a partially overlaps with the gate conductor layer 4 ab via an insulting layer 18 ab covering the gate conductor layer 4 ab.

With the above structure, there is no gap between the gate conductor layer 4 ab and first conductor layer 13 ab, therefore, no leakage of light through such a gap occurs. Hence, leakage of light into an adjacent pixel can effectively be prevented. Consequently, the solid state imaging device of this embodiment can effectively prevent deteriorated resolution and mixed color.

Embodiment 9

A solid state imaging device according to Embodiment 9 of the present invention will be described hereafter with reference to FIG. 12. The same components as those of Embodiment 5 are referred to by the same reference numbers. FIG. 12 is an enlarged view of a region including the second semiconductor P layers 2 a and 2 b, gate conductor layers 4 ab and 4 ba, third semiconductor N layers 5 ab and 5 ba, fourth semiconductor P⁺ layers 6 ab and 6 ba, and fifth semiconductor P⁺ layers 7 a and 7 b of the pixel structure of the solid state imaging device of Embodiment 5. This embodiment is different from Embodiment 5 in that the first conductor layers 13 ab and 13 ba partially overlap with the gate conductor layers 4 ab and 4 ba, respectively, via insulting layers 18 ab and 18 ba covering the gate conductor layers 4 ab and 4 ba.

With the above structure, as in the solid state imaging device of Embodiment 8, leakage of light into an adjacent pixel can effectively be prevented. Consequently, the solid state imaging device of this embodiment can effectively prevent deteriorated resolution and mixed color.

A method of producing the solid state imaging device according to Embodiment 9 will be described hereafter with reference to FIGS. 13 to 21.

First, as shown in FIG. 13, a P-type silicon layer 301, a silicon nitride layer 302, and a silicon oxide layer 303 are deposited on a silicon (SiO₂) substrate. Then, as shown in FIG. 14, island-shaped semiconductor layers 304 a and 304 b are formed by etching. Then, for example, the substrate is heated in an oxygen atmosphere to oxidize the silicon surface and form a silicon oxide film 305. Then, polysilicon film is deposited and etched back to form a polysilicon sidewall film 306 as shown in FIG. 15.

Then, phosphorus ions are implanted in the P-type silicon layer 301 by ion implantation to form the first semiconductor N⁺ layers 1 a and 1 b. Then, the polysilicon film 306 and silicon oxide film 305 are etched off. Then, a silicon oxide film layer 307 is formed. A gate oxide film 308 is formed by gate oxidation. A polysilicon film 309 is deposited by CVD of thermal decomposition of monosilane as shown in FIG. 16. Then, a silicon oxide film (SiO₂film) 310 is formed on the polysilicon film 309 in the region where the first gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb are defined. Then, the polysilicon film 309 other than the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb is removed by etching using the SiO₂film 310 or a resist film as a mask, whereby the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb are formed as shown in FIG. 17. Then, the SiO₂film 310 is removed and the polysilicon of the gate conductor layers 4 aa, 4 ab, 4 ba, and 4 bb is oxidized to form the insulating films 18 aa, 18 ab, 18 ba, and 18 bb.

Then, phosphorus ions are implanted in the P-type silicon layer 301 by ion implantation to form the third semiconductor N-layers 5 aa, 5 ab, 5 ba, and 5 bb. Boron ions are further implanted in the third semiconductor N-layers 5 aa, 5 ab, 5 ba, and 5 bb by ion implantation to form the fourth semiconductor P⁺ layers 6 aa, 6 ab, 6 ba, and 6 bb as shown in FIG. 18. Then, the silicon nitride film 302 is removed. Then, silicon oxide or silicon nitride is deposited, flattened, and etched back to form a silicon oxide film 311 a. The exposed semiconductor layer is oxidized to form a silicon oxide film 312. Boron is implanted to form the fifth semiconductor P⁺ layers 7 a, 7 b as shown in FIG. 19. Then, the silicon oxide film 312 is peeled off. The silicon oxide film 311 a is removed by etching to the depth at which the first conductor layers 13 ab and 13 ba and the gate conductor layers 4 ab and 4 ba of the MOS transistors overlap with each other so as to form a silicon oxide film 311 b as shown in FIG. 20. Then, the polysilicon of the gate conductor layers 4 ab and 4 ba is oxidized. Then, a metal film is formed on the entire surface of the substrate by vacuum deposition or sputtering and patterned to form the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb and the first wiring conductor layers 14 a, 14 b, and 14 c. The first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb are joined to the fifth semiconductor P⁺ layers and the first wiring conductor layers 14 a, 14 b, and 14 c connect the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb to each other.

The pixel structure of the solid state imaging device of Embodiment 9 is obtained in the above process. Furthermore, the pixel structure of the solid state imaging device of Embodiment 8 is obtained by patterning the metal film as shown in FIG. 11 in the step of forming the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb and first wiring conductor layers 14 a, 14 b, and 14 c.

Embodiment 10

In a conventional solid state imaging device, the pixels, circuits driving the pixels, circuits retrieving signals from the pixels are formed on one and the same substrate. It is preferable that these circuits also have a three-dimensional structure in the solid state imaging devices according to Embodiments 1 to 9 having three-dimensionally structured pixels. For example, these circuits can consist of a SGT (surrounding gate transistor) described in H. Takato, K. Sunouchi, N. Okabe, A. Nitayama, K. Hieda, F. Horiguchi, F. Masuoka: “Impact of Surrounding Gate Transistor (SGT) for Ultra-High-Density LSI's”, IEEE Transactions on Electron devices, Vol. 38, No. 3, pp. 573-578 (1991). Such a solid state imaging device will be described hereafter as Embodiment 10 with reference to FIG. 22. FIG. 22 is a cross-sectional view of a solid state imaging device according to Embodiment 10.

The solid state imaging device according to this embodiment comprises a substrate 400, one or multiple pixels 11 g formed on the substrate 400, and a pixel drive and/or output circuit 401 formed on the substrate 400 for driving the pixel 11 g and/or retrieving signals from the pixel 11 g. The pixel 11 g has the same pixel structure as the pixel 11 in Embodiment 1. The pixel drive and/or output circuit 401 comprises a CMOS circuit consisting of an N channel MOS transistor part 402 a and a P channel MOS transistor part 402 b. Here, the pixel drive and/or output circuit 401 represents a collection of the above-described vertical scanning circuit, horizontal scanning circuit, reset circuit, and correlated double sampling output circuit.

The N channel MOS transistor part 402 a is composed of a semiconductor substrate layer 403 a formed on the substrate 400, a P well layer 406 a formed on the semiconductor substrate layer 403 a, and one or multiple N

channel MOS transistors

404 a and 404 b formed on the P well layer 406 a. The N

channel MOS transistors

404 a and 404 b are each composed of a semiconductor column 408 and 408 b, a

gate insulating layer

409 a and 409 b, a

gate conductor layer

410 a and 410 b, and source/drain N⁺ layers 407 a and 407 b, respectively. The

gate insulating layers

409 a and 409 b surround the

semiconductor columns

408 a and 408 b, respectively. The gate conductor layers 410 a and 410 b are formed on the

gate insulating layers

409 a and 409 b so as to surround the

semiconductor columns

408 a and 408 b, respectively. The source/drain N⁺ layers 407 a are formed on the top and the bottom of the semiconductor column 408 a. The source/drain N⁺ layers 407 b are formed on the top and the bottom of the semiconductor column 408 b. The N channel MOS transistor part 402 a is formed in the manner that the height of the N channel MOS transistor part 402 a between the substrate 400 and the uppermost source/drain N⁺ layers 407 a and 407 b is equal to the height of the pixel 11 g between the substrate 400 and the fifth semiconductor layer or P⁺ layer 7. The P well layer 406 a is connected to the power source and receives a P well voltage. The

semiconductor columns

408 a and 408 b between the source/drain N⁺ layers 407 a and 407 b serve as a channel for the N

channel MOS transistors

404 a and 404 b, respectively.

The P channel MOS transistor part 402 b is composed of a semiconductor substrate layer 403 b formed on the substrate 400, an N well layer 406 b formed on the semiconductor substrate layer 403 b, and one or multiple P

channel MOS transistors

405 a and 405 b formed on the N well layer 406 b. The P

channel MOS transistors

405 a and 405 b are each composed of a

semiconductor column

412 a and 412 b, a

gate insulating layer

413 a and 413 b, a

gate conductor layer

414 a and 414 b, and source/drain P⁺ layers 411 a and 411 b, respectively. The

gate insulating layers

413 a and 413 b surround the

semiconductor columns

412 a and 412 b, respectively. The gate conductor layers 414 a and 414 b are formed on the

gate insulating layers

413 a and 413 b so as to surround the

semiconductor columns

412 a and 412 b, respectively. The source/drain P⁺ layers 411 a are formed on the top and the bottom of the semiconductor column 412 a. The source/drain P⁺ layers 411 b are formed on the top and the bottom of the semiconductor columns 412 b. The P channel MOS transistor part 402 b is formed in the manner that the height of the P channel MOS transistor part 402 b between the substrate 400 and the uppermost source/drain P⁺ layers 411 a and 411 b is equal to the height of the pixel 11 g between the substrate 400 and the fifth semiconductor layer or P⁺ layer 7. The N well layer 406 b is connected to the power source and receives an N well voltage. The

semiconductor columns

412 a and 412 b between the source/drain P⁺ layers 411 a or 411 b serve as a channel for the P

channel MOS transistors

405 a and 405 b, respectively.

The

MOS transistors

404 a, 404 b, 405 a, and 405 b constituting the N channel and P channel

MOS transistor parts

402 a and 402 b are electrically connected to each other, to the power source, or to the ground via wiring to form a CMOS circuit. Furthermore, the pixel drive and/or output circuit 401 is electrically connected to the pixel 11 g via wiring.

With the above structure, the pixel 11 g and the MOS transistors constituting the pixel drive and/or output circuit 401 are three-dimensionally constructed on one and the same substrate 400. Compared with the use of planar MOS transistors, the mounting area of the pixel 11 g and pixel drive and/or output circuit 401 on the substrate 400 can be reduced. Then, the pixels can be provided at a higher density and a compact solid state imaging device can be realized. Furthermore, with the above structure, the N channel MOS transistor part 402 a, P channel MOS transistor part 402 b, and pixel 11 g have the same height. The semiconductor columns serving as their body can be formed in the same step without adjusting individual etching or polishing conditions. Then, the solid state imaging device having the above structure according to Embodiment 10 can be produced by a simplified production process compared with the prior art solid state imaging device.

Embodiment 11

In the solid state imaging device according to Embodiment 10, the N channel MOS transistors and P channel MOS transistors are collectively formed on the P well layer and N well layer, respectively. Alternatively, they can individually be formed on the substrate. Such a solid state imaging device will be described as Embodiment 11 with reference to FIG. 23. FIG. 23 is a cross-sectional view of a solid state imaging device according to Embodiment 11.

The solid state imaging device according to this embodiment comprises a substrate 400, one or multiple pixels 11 h formed on the substrate 400, and a pixel drive and/or output circuit 401 formed on the substrate 400 for driving the pixel 11 h and/or retrieving signals from the pixel 11 h. The pixel 11 h has the same pixel structure as the pixel 11 f in Embodiment 3. In other words, in the pixel 11 h, the gate conductor layers 4 ba and 4 bb of a MOS transistor for reset operation is extended to cover the photodiode surface P⁺ layer (the fourth semiconductor layer or P⁺ layer) 6 ba and 6 bb. The pixel drive and/or output circuit 401 comprises a CMOS circuit consisting of an N channel MOS transistor part 402 a and a P channel MOS transistor part 402 b.

The N channel MOS transistor part 402 a is composed of one or multiple N

channel MOS transistors

415 a and 415 b formed on the substrate 400. The N

channel MOS transistors

415 a and 415 b are each composed of a

semiconductor column

417 a and 417 b, a

gate insulating layer

418 a and 418 b, a

gate conductor layer

419 a and 419 b, and source/drain N⁺ layers 416 a and 416 b, respectively. The

gate insulating layers

418 a and 418 b surround the

semiconductor columns

417 a and 417 b, respectively. The gate conductor layers 419 a and 419 b are so formed on the

gate insulating layers

418 a and 418 b as to surround the

semiconductor columns

417 a and 417 b, respectively, and have the same height as the gate conductor layers 4 ba and 4 bb of the pixel 11 h. The source/drain N⁺ layers 416 a are formed on the top and the bottom of the semiconductor columns 417 a. The source/drain N⁺ layers 416 b are formed on the top and the bottom of the semiconductor columns 417 b. The N

channel MOS transistors

415 a and 415 b are formed in the manner that the height of the N

channel MOS transistors

415 a and 415 b between the substrate 400 and the uppermost source/drain N⁺ layers 416 a and 416 b is the same as the height of the pixel 11 h between the substrate 400 and the firth semiconductor layer or P⁺ layer 7 b. The

semiconductor columns

417 a and 417 b between the source/drain N⁺ layers 416 a or 416 b serve as a channel for the N

channel MOS transistors

415 a and 415 b, respectively.

The P channel MOS transistor part 402 b is composed of one or multiple P

channel MOS transistors

420 a and 420 b formed on the substrate 400. The P

channel MOS transistors

420 a and 420 b are each composed of a

semiconductor column

422 a and 422 b, a

gate insulating layer

423 a and 423 b, a

gate conductor layer

424 a and 424 b, and source/drain P⁺ layers 421 a and 421 b, respectively. The

gate insulating layers

423 a and 423 b surround the

semiconductor columns

422 a and 422 b, respectively. The gate conductor layers 424 a and 424 b are so formed on the

gate insulating layers

423 a and 423 b as to surround the

semiconductor columns

422 a and 422 b, respectively, and have the same height as the gate conductor layers 4 ba and 3 bb of the pixel 11 h. The source/drain P⁺ layers 421 a are formed on the top and the bottom of the semiconductor columns 422 a. The source/drain P⁺ layers 421 b are formed on the top and the bottom of the semiconductor columns 422 b. The P

channel MOS transistors

420 a and 420 b are formed in the manner that the height of the P

channel MOS transistors

420 a and 420 b between the substrate 400 and the uppermost source/drain P⁺ layers 421 a and 421 b is the same as the height of the pixel 11 h between the substrate 400 and the firth semiconductor layer or P⁺ layer 7 b. The

semiconductor columns

422 a and 422 b between the source/drain P⁺ layers 421 a or 421 b serve as a channel for the P

channel MOS transistors

420 a and 420 b, respectively.

The

MOS transistors

415 a, 415 b, 420 a, and 420 b constituting the N channel and P channel

MOS transistor parts

402 a and 402 b are electrically connected to each other, to the power source, or to the ground via wiring to form a CMOS circuit. Furthermore, the pixel drive and/or output circuit 401 is electrically connected to the pixel 11 h via wiring.

With the above structure, the pixel 11 h and the MOS transistors constituting the pixel drive and/or output circuit 401 are three-dimensionally constructed on one and the same substrate 400. Compared with the use of planar MOS transistors in constructing the pixel drive and/or output circuit, the mounting area of the pixel 11 h and pixel drive and/or output circuit 401 on the substrate 400 can be reduced. Then, the pixels can be provided at a higher density and a compact solid state imaging device can be realized. Furthermore, with the above structure, the N

channel MOS transistors

415 a and 415 b, P

channel MOS transistors

420 a and 420 b, and pixel 11 h have the same height. The semiconductor columns serving as their body can be formed in the same step without adjusting individual etching or polishing conditions. Similarly, the gate conductor layers 419 a, 419 b, 424 a, and 424 b and the gate conductor layers 4 ba and 4 bb of the pixel 11 h have the same height. They can be formed in the same step without adjusting individual etching or polishing conditions for each gate conductor layer. Then, the solid state imaging device having the above structure according to Embodiment 11 can be produced by a simplified production process compared with the solid state imaging device according to Embodiment 10. Furthermore, in order to set the voltages of the

MOS transistors

415 a, 415 b, 420 a, and 420 b at a given threshold voltage, either the gate conductor layers 419 a and 419 b of the N

channel MOS transistors

415 a and 415 b or the gate conductor layers 424 a and 424 b of the P

channel MOS transistors

420 a and 420 b can be formed as the gate conductor layers 4 ba and 4 bb of the pixel 11 h. Then, the solid state imaging device can be produced by a simplified production process compared with Embodiment 10.

Modified Embodiments

In the above Embodiments 1 to 9, the explanation is made as to the case wherein the first semiconductor layer is an N⁺ layer. The same effect can be obtained in a solid state imaging device in which the polarities of the semiconductor layers are reversed, i.e. the first semiconductor layer is a P⁺ layer, the second semiconductor layer is an N layer, the third semiconductor layer is a P layer, the fourth semiconductor layer on the photodiode surface is an N⁺ layer, and the fifth semiconductor layer is an N⁺ layer.

Furthermore, in the above Embodiments 1 to 6, 8, and 9, the wire joined to the first semiconductor N⁺ layer 1 and the wire joined to the fifth semiconductor P⁺ layer 7 are orthogonal to each other. They are not necessarily orthogonal to each other when the first semiconductor N⁺ layer 1 is exclusively used as a drain for removing signal charges during the reset operation.

In the above Embodiment 2, the depleted layer 8 c of the photodiode 112 occupies the upper region of the second semiconductor P layer 2 where the photodiode 112 is formed when no signal charges are accumulated in the photodiode region during the signal reading. If the depleted layer 8 c of the photodiode 112 occupies the upper region of the second semiconductor P layer 2 even when a tiny amount of signal charges are accumulated in the photodiode region, the tiny amount of signal chare is not output as a signal. Therefore, the amplifying junction transistor may be designed to establish a channel in the photodiode region within an allowable range of operational margin.

In the above Embodiments 1 to 9, the explanation is made with one or two pixels. Needless to say, the present invention can be applied to a solid state imaging device in which the pixels are arranged in one-dimensional or two-dimensional array.

In the above Embodiments 1 to 9, the pixels can be arranged in a linear or zigzag pattern in the case of one-dimensional array and arranged in a linear lattice or honeycomb pattern in the case of two-dimensional array although they are not restricted thereto.

In the above Embodiments 1 to 9, at least the region where the photodiode 112 is formed (the upper region of the second semiconductor P layer 2 where the third

semiconductor N layer

5 a, 5 b are formed and the third

semiconductor N layer

5 a, 5 b), fourth semiconductor P⁺ layer, and fifth semiconductor P⁺ layer are formed in the shape of an island. This island-shaped semiconductor can be cylindrical, hexagonal, or in other shapes.

In the above Embodiments 5 to 7 and 9, the first conductor layers 13 aa, 13 ab, 13 ba, and 13 bb, first wiring conductor layers 14 a to 14 c, second wiring conductor layers 15 a to 15 c, and second conductor layers (filling conductor layers) 16 a to 16 c and 17 a to 17 c are distinguished in material. However, the same effect can be obtained even if they are made of the same material.

In the above Embodiments 1 to 9, the explanation is made as to solid state imaging devices generating signal charges in pixels upon light irradiation. Needless to say, the present invention can be applied to solid state imaging devices generating signal charges in pixels upon irradiation of electromagnetic energy waves such as visible light, ultraviolet light, infrared light, X-ray, other electromagnetic ray, radioactive ray, and an electron beam.

In the above Embodiment 7, the space between pixels is filled with the second conductor layers 16 a to 16 c and 17 a to 17 c to efficiently prevent leakage of light between pixels. The same effect can be obtained by filling with a conductor layer between the gate conductor layers 4 a and 4 b of the MOS transistors 111 of pixels of the solid state imaging device according to Embodiment 1.

In the above Embodiments 1 to 9, the second semiconductor P layer 2 serves as the channel of the MOS transistor 111. For example, an impurity can be implanted in a region of the second semiconductor P layer 2 by ion implantation to form a channel.

Furthermore, the first semiconductor layer 1 can be formed continuously over pixels or formed for each pixel. When the first semiconductor is formed for each pixel, the first semiconductor layers 1 can be connected each other by another metal wiring. The first and

second semiconductor layers

1 and 2 do not need to be in contact with (jointed to) each other at the entire surface and can be in contact in part. Furthermore, the first semiconductor layer 1 can partly be replaced with another semiconductor layer.

In the above Embodiments 1 to 9, the conductor layers such as the

gate conductor layer

4 a, 4 b of the MOS transistor 111 are made of a single material. For example, they can be composed of multiple layers such as metal layers and polycrystalline silicon layer.

In the above Embodiments 10 and 11, the pixel drive and/or output circuit 401 comprises a vertical scanning circuit, horizontal scanning circuit, reset circuit, and correlated double sampling circuit and may comprise other circuits for controlling the pixel. For example, the pixel drive and/or output circuit 401 may comprise a signal preprocessing circuit provided next to each pixel or a MOS transistor controlling the timing of retrieving pixel signals.

In the above Embodiments 10 and 11, the fifth semiconductor or P⁺ layer 7 or 7 b and some of the source/drain layers 407 a, 407 b, 411 a, 411 b, 416 a, 416 b, 421 a, and 412 b formed above the

semiconductor columns

408 a, 408 b; 412 a, 412 b, 417 a, 417 b, 422 a, and 422 b of the N channel and P channel

MOS transistor parts

402 a and 402 b of a pixel can separately be formed by ion implantation and epitaxial growth. In such a case, there may be a slight difference in the position in the height direction between the fifth semiconductor or P⁺ layer 7 or 7 b and the source/drain layers 407 a, 407 b, 411 a, 411 b, 416 a, 416 b, 421 a, and 412 b formed above the

semiconductor columns

408 a, 408 b, 412 a, 412 b, 417 a, 417 b, 422 a, and 422 b of the N channel and P channel

MOS transistor parts

402 a and 402 b. However, the effect and benefit of the present invention is not impaired. For example, even in a solid state imaging device according to this modified embodiment, the semiconductor columns serving as the body of the N channel MOS transistor part 402 a, P channel MOS transistor part 402 b, and

pixel

11 g or 11 h can be formed in the same step without adjusting individual etching or polishing conditions as in the solid state imaging devices according to Embodiments 10 and 11.

Having described and illustrated the principles of this application by reference to one (or more) preferred embodiment(s), it should be apparent that the preferred embodiment(s) may be modified in arrangement and detail without departing from the principles disclosed herein and that it is intended that the application be construed as including all such modifications and variations insofar as they come within the spirit and scope of the subject matter disclosed herein.

Claims

What is claimed is:

1. A solid state imaging device including one or multiple pixels, each of the pixels comprising:

a first semiconductor layer formed on a substrate,

a second semiconductor layer formed on the first semiconductor layer,

a first insulating film formed on a lower side of the second semiconductor layer,

a gate conductor layer formed on the lower side of the second semiconductor layer via the first insulating film,

a third semiconductor layer formed in an upper side of the second semiconductor layer,

a fourth semiconductor layer formed on a side of the third semiconductor layer that is not facing a side of the second semiconductor layer, and

a fifth semiconductor layer formed on top of the second semiconductor layer and the third semiconductor layer, the fifth semiconductor layer electrically connected to the fourth semiconductor layer,

wherein

at least the third semiconductor layer, the upper region of the second semiconductor layer where the third semiconductor layer is formed, the fourth semiconductor layer, and the fifth semiconductor layer are formed in an island,

a diode comprises the second semiconductor layer and the third semiconductor layer,

a junction transistor comprises the diode serving as a gate thereof and the second semiconductor layer serving as a channel thereof, the channel being between the first semiconductor layer and the fifth semiconductor layer,

a MOS transistor comprises the gate semiconductor layer serving as a gate thereof and the second semiconductor layer serving as a channel thereof, the channel being between the first semiconductor layer and the third semiconductor layer,

a signal charge generated by an electromagnetic energy wave is accumulated in the diode,

current flowing to the junction transistor and changing in accordance with amount of the signal charge accumulated in the diode is detected as a signal,

the signal charge accumulated in the diode is removed at the first semiconductor layer through the MOS transistor channel,

the fourth semiconductor layer and the fifth semiconductor layer have same voltage.

2. The solid state imaging device according to claim 1 wherein,

the second semiconductor layer is a conductivity type opposite to the conductivity type of the first semiconductor layer, or a substantially intrinsic type,

the third semiconductor layer has a conductivity type the same as a conductivity type of the first semiconductor layer,

the fourth semiconductor layer has a conductivity type opposite to a conductivity type of the first semiconductor layer,

the fifth semiconductor layer has a conductivity type opposite to a conductivity type of the first semiconductor layer, and

the fourth and fifth semiconductor layers are connected to each other.

3. The solid state imaging device according to claim 1, further comprising a first conductor layer formed on the side of the fourth semiconductor layer via the first insulating film so as to enclose the third semiconductor layer, an upper region of the second semiconductor layer, and the fourth semiconductor layer in the shape of the island, the first conductor layer including a light-blocking conductive material,

wherein the first conductor layer is connected to the fifth semiconductor layer.

4. The solid state imaging device according to claim 3, further comprising:

a gap between the first conductor layer and the gate conductor layer; and

a first wiring conductor layer connecting the first conductor layers of adjacent pixels in a space near the gap between the first conductor layer and the gate conductor layer, the space being between the pixels, and the first wiring conductor layer including a light-blocking conductive material.

5. The solid state imaging device according to claim 3, further comprising a second insulating film covering the gate conductor layer,

wherein the first conductor layer overlaps with at least part of the gate conductor layer via the second insulating film.

6. The solid state imaging device according to claim 3, further comprising:

a gap between the first conductor layer and the gate conductor layer; and

a second wiring conductor layer connecting the gate conductor layers of adjacent pixels in a space near the gap between the first conductor layer and the gate conductor layer, the space being between the pixels, and the second wiring conductor layer including a light-blocking conductive material.

7. The solid state imaging device according to claim 3, further comprising:

a second conductor layer filling between the first conductor layers of adjacent pixels, between the gate conductor layers of adjacent pixels, or between the first conductor layers of adjacent pixels and between the gate conductor layers of adjacent pixels, and the second conductor layer including a light-blocking conductive material.

8. The solid state imaging device according to claim 1, wherein

the gate conductor layer extends onto the side of the fourth semiconductor layer via the first insulating film so as to enclose the third semiconductor layer, an upper region of the second semiconductor layer, and the fourth semiconductor layer in the shape of the island, the gate conductor layer including a light-blocking conductive material.

9. The solid state imaging device according to claim 1 comprising:

a unit for accumulating a signal charge in the third semiconductor layer and the second semiconductor layer near the third semiconductor layer according to a quantity of electromagnetic energy wave irradiation;

a signal reading unit for measuring a current running between the fifth semiconductor layer and the second semiconductor layer near the first semiconductor layer so as to measure the accumulated signal charge for reading signals; and

a reset unit for applying an ON voltage to the gate conductor layer to create a channel in a region including the second semiconductor layer between the first semiconductor layer and the third semiconductor layer, whereby the signal charge accumulated in the third semiconductor layer is discharged to the first semiconductor layer and removed,

wherein

the signal reading unit sets potentials so that the potentials become deeper in a following order: the potential of the first semiconductor layer; the potential of the fifth semiconductor layer; and the deepest potential in the third semiconductor layer, the deepest potential in the third semiconductor layer being a potential when no signal charge is accumulated in the third semiconductor layer and the second semiconductor layer near the third semiconductor layer, and

the reset unit sets potentials so that the potentials become deeper in a following order: the potential of the fifth semiconductor layer; the deepest potential in the third semiconductor layer; the potential of a channel in a region including the second semiconductor layer between the first semiconductor layer and the third semiconductor layer when an ON voltage is applied to the gate conductor layer; and the potential of the first semiconductor layer, the deepest potential in the third semiconductor layer being a potential when no signal charge is accumulated in the third semiconductor layer and the second semiconductor layer near the third semiconductor layer.

10. The solid state imaging device according to claim 9, wherein

in a relationship of the potentials set by the signal reading unit, a depleted layer formed in an upper region of the second semiconductor layer occupies the upper region of the second semiconductor layer when no signal charge is accumulated in the third semiconductor layer and the second semiconductor layer near the third semiconductor layer, the third semiconductor layer being formed in the upper region of the second semiconductor layer, and

in a relationship of the potentials set by the signal reading unit, a thickness of the depleted layer varies according to the accumulated signal charge when the signal charge is accumulated in the third semiconductor layer and the second semiconductor layer near the third semiconductor layer.

11. The solid state imaging device according to claim 1, comprising a pixel drive/output unit driving the pixel and retrieving signals from the pixel, wherein

the pixel drive/output unit is composed of multiple surrounding gate transistors.

12. The solid state imaging device according to claim 3, comprising a pixel drive/output unit driving the pixel and retrieving signals from the pixel, wherein

the pixel drive/output unit is composed of multiple surrounding gate transistors,

each of the surrounding gate transistors each comprises a gate conductor layer, and

the gate conductor layers of the multiple surrounding gate transistors and the first conductor layers of the one or multiple pixels have the same height.